Math 2.0

Mechanics of deformable solids Definition

Lamé parameters

Builds on Elasticity tensorStrain tensorCauchy stress tensorOrthogonal matrix

Definition

An elasticity tensor CC is isotropic if QipQjqQkrQlsCpqrs=CijklQ_{ip} Q_{jq} Q_{kr} Q_{ls} C_{pqrs} = C_{ijkl} for every orthogonal matrix QQ, with summation over repeated indices. Every isotropic elasticity tensor has the form Cijkl=λ δijδkl+μ (δikδjl+δilδjk)C_{ijkl} = \lambda \, \delta_{ij} \delta_{kl} + \mu \, (\delta_{ik} \delta_{jl} + \delta_{il} \delta_{jk}) for unique real numbers λ\lambda and μ\mu, where δ\delta is the Kronecker delta. These numbers are the Lamé parameters of CC: λ\lambda is the first Lamé parameter and μ\mu is the second. Equivalently, the stress produced by a strain ε\varepsilon is the stress σ=λ(tr⁡ε)I+2με\sigma = \lambda (\tr \varepsilon) I + 2\mu \varepsilon.

Remarks

Example: with λ=1\lambda = 1 and μ=1\mu = 1 and the pure shear strain ε=γ(e1⊗e2+e2⊗e1)/2\varepsilon = \gamma (e_1 \otimes e_2 + e_2 \otimes e_1)/2, the trace is 00 and σ12=2μ⋅γ/2=γ\sigma_{12} = 2\mu \cdot \gamma/2 = \gamma; so μ\mu is the ratio of shear stress to engineering shear strain γ\gamma.

Non-example: a cubic crystal has an elasticity tensor with three independent constants, and in general it is not of the form above, so it has no Lamé parameters.

Positivity of the elasticity tensor is equivalent to μ>0\mu > 0 and 3λ+2μ>03\lambda + 2\mu > 0. In terms of Young's modulus EE and Poisson's ratio ν\nu, λ=Eν(1+ν)(1−2ν)\lambda = \frac{E \nu}{(1 + \nu)(1 - 2\nu)} and μ=E2(1+ν)\mu = \frac{E}{2(1 + \nu)}.

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  1. Cauchy stress tensor concept
  2. Elasticity tensor concept
  3. Orthogonal matrix concept
  4. Strain tensor concept
  5. Lamé parameters definition

Further reading

  1. Web https://en.wikipedia.org/wiki/Lam%C3%A9_parameters
About this page
Tag5Y441DTXN0
URIm2://5Y441DTXN0
Kinddefinition
WritingW0 stub
MSC74B05
DefinesLamé parameters
UsesElasticity tensor, Strain tensor, Cauchy stress tensor, Orthogonal matrix
Changed3 November 2026

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